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Practical_Antenna_Handbook_0071639586

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C h a p t e r 2 : r a d i o - W a v e P r o p a g a t i o n 55<br />

Ionosphere<br />

Signal<br />

refracts<br />

T time for round trip<br />

H 3 108 m/s T<br />

2<br />

Virtual<br />

height<br />

(H)<br />

Earth's surface<br />

Transmitter<br />

Figure 2.31 Finding the virtual height of the ionosphere.<br />

other hand, will depend on the state of the ionosphere 2500 mi away from the site<br />

where f C is measured, so the two indices do not track perfectly.<br />

On average, the best propagation occurs at frequencies just below the MUF. In fact,<br />

the frequency of optimum traffic (FOT) is approximately 85 percent of the MUF. Near the<br />

FOT, signal strengths are optimum because ionospheric absorption is at a minimum<br />

and signal-to-noise ratios (SNRs) are highest because atmospheric noise generally decreases<br />

with increasing frequency.<br />

Lowest Useable Frequency (LUF)<br />

Below a certain frequency, the combination of ionospheric absorption and atmospheric<br />

noise, static, etc., conspire to hinder and even prevent radio communications. The lowest<br />

useable frequency (LUF) is a measure intended to help identify the lower frequency<br />

limit for successful communications.<br />

Unlike the MUF, the LUF is not dependent solely on atmospheric physics. The LUF<br />

of a system can be varied by controlling the signal-to-noise ratio of the transmitterreceiver<br />

path. Although many of the factors that contribute to SNRs are beyond our<br />

control, the effective radiated power (ERP) of the transmitter is one that often can be<br />

changed. For instance, a 2-MHz decrease in LUF is available for every 10-dB increase in<br />

the ERP of the transmitter. In practice, this can be accomplished through the use of

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